JPS63111602A - High performance rare earth cast magnet - Google Patents
High performance rare earth cast magnetInfo
- Publication number
- JPS63111602A JPS63111602A JP61256743A JP25674386A JPS63111602A JP S63111602 A JPS63111602 A JP S63111602A JP 61256743 A JP61256743 A JP 61256743A JP 25674386 A JP25674386 A JP 25674386A JP S63111602 A JPS63111602 A JP S63111602A
- Authority
- JP
- Japan
- Prior art keywords
- rare earth
- magnet
- magnets
- cast
- magnetic properties
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 229910052761 rare earth metal Inorganic materials 0.000 title claims abstract description 15
- 150000002910 rare earth metals Chemical class 0.000 title claims abstract description 11
- 239000000203 mixture Substances 0.000 claims abstract description 11
- 229910052726 zirconium Inorganic materials 0.000 claims abstract description 6
- 229910052802 copper Inorganic materials 0.000 claims abstract description 5
- 229910052758 niobium Inorganic materials 0.000 claims abstract description 5
- 229910052735 hafnium Inorganic materials 0.000 claims abstract description 4
- 229910052748 manganese Inorganic materials 0.000 claims abstract description 4
- 229910052759 nickel Inorganic materials 0.000 claims abstract description 4
- 229910052782 aluminium Inorganic materials 0.000 claims abstract description 3
- 229910052750 molybdenum Inorganic materials 0.000 claims abstract description 3
- 229910052715 tantalum Inorganic materials 0.000 claims abstract description 3
- 229910052719 titanium Inorganic materials 0.000 claims abstract description 3
- 229910052720 vanadium Inorganic materials 0.000 claims abstract description 3
- 229910052721 tungsten Inorganic materials 0.000 claims abstract 2
- 229910052799 carbon Inorganic materials 0.000 claims 1
- 238000000034 method Methods 0.000 abstract description 36
- 238000005266 casting Methods 0.000 abstract description 15
- XEEYBQQBJWHFJM-UHFFFAOYSA-N iron Substances [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 abstract description 10
- 238000010791 quenching Methods 0.000 abstract description 9
- 230000000171 quenching effect Effects 0.000 abstract description 9
- 229910000828 alnico Inorganic materials 0.000 abstract description 8
- 239000000654 additive Substances 0.000 abstract description 7
- 239000000843 powder Substances 0.000 abstract description 7
- 238000001816 cooling Methods 0.000 abstract description 6
- 229910052796 boron Inorganic materials 0.000 abstract description 4
- 229910052742 iron Inorganic materials 0.000 abstract description 4
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 abstract description 3
- 229910052804 chromium Inorganic materials 0.000 abstract description 3
- 239000000463 material Substances 0.000 abstract description 2
- 229910045601 alloy Inorganic materials 0.000 description 9
- 239000000956 alloy Substances 0.000 description 9
- 238000004663 powder metallurgy Methods 0.000 description 8
- 230000007423 decrease Effects 0.000 description 7
- 230000004907 flux Effects 0.000 description 7
- 238000005245 sintering Methods 0.000 description 7
- 238000004519 manufacturing process Methods 0.000 description 4
- 230000003647 oxidation Effects 0.000 description 4
- 238000007254 oxidation reaction Methods 0.000 description 4
- 239000011347 resin Substances 0.000 description 4
- 229920005989 resin Polymers 0.000 description 4
- 230000000996 additive effect Effects 0.000 description 3
- 229910017052 cobalt Inorganic materials 0.000 description 3
- 239000010941 cobalt Substances 0.000 description 3
- GUTLYIVDDKVIGB-UHFFFAOYSA-N cobalt atom Chemical compound [Co] GUTLYIVDDKVIGB-UHFFFAOYSA-N 0.000 description 3
- 239000010949 copper Substances 0.000 description 3
- 238000010438 heat treatment Methods 0.000 description 3
- 238000000465 moulding Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 238000003754 machining Methods 0.000 description 2
- 229910052751 metal Inorganic materials 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 229910018106 Ni—C Inorganic materials 0.000 description 1
- 230000032683 aging Effects 0.000 description 1
- 238000005275 alloying Methods 0.000 description 1
- 230000000052 comparative effect Effects 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 239000002178 crystalline material Substances 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000007731 hot pressing Methods 0.000 description 1
- 239000012770 industrial material Substances 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 238000002156 mixing Methods 0.000 description 1
- 230000001590 oxidative effect Effects 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 238000010298 pulverizing process Methods 0.000 description 1
- 239000002994 raw material Substances 0.000 description 1
- 239000004576 sand Substances 0.000 description 1
- 238000006467 substitution reaction Methods 0.000 description 1
- 229910052723 transition metal Inorganic materials 0.000 description 1
- 150000003624 transition metals Chemical class 0.000 description 1
- 229910000859 α-Fe Inorganic materials 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/032—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials
- H01F1/04—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials metals or alloys
- H01F1/047—Alloys characterised by their composition
- H01F1/053—Alloys characterised by their composition containing rare earth metals
- H01F1/055—Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5
- H01F1/057—Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B
Landscapes
- Chemical & Material Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- Inorganic Chemistry (AREA)
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Hard Magnetic Materials (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は希土類−鉄−ホウ素系永久磁石(以下、R−F
e−B系磁石という)に関するものであり、さらに詳し
く述べるならば鋳造により高性能を達成したR−Fe−
B系磁石に関するものである。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to rare earth-iron-boron permanent magnets (hereinafter referred to as R-F
e-B series magnets), and in more detail, R-Fe- which achieved high performance through casting.
This relates to B-based magnets.
R−Fe−B系磁石は、高価なコバルト等を必須成分と
せずにまた安価な工業材料である鉄を多量に用いること
によって、優れた磁石特性を実現する。これまで、より
一層の磁石特性の向上を図り、より安価な元素を使用し
つつ良好な磁石特性を達成し、あるいは加工性を向上す
る等の方法によって、従来の一般的永久磁石である希土
類コバルト永久磁石、フェライト磁石に代替しあるいは
これらの磁石と競合できるR−Fe−B系磁石を提供す
るための研究が活発になされている。R-Fe-B magnets achieve excellent magnetic properties by not using expensive cobalt or the like as an essential component and by using a large amount of iron, which is an inexpensive industrial material. Up until now, efforts have been made to further improve magnetic properties, achieve good magnetic properties while using cheaper elements, or improve workability, thereby reducing the amount of rare earth cobalt that is conventionally used in general permanent magnets. Research is being actively conducted to provide R--Fe--B magnets that can replace or compete with permanent magnets and ferrite magnets.
R−Fe−B系磁石については、各種製造方法が示され
ているが、それらは主に次の2つに大別される。1つは
、特開昭59−64739号公報で発表された高速急冷
法を用いたものである。この方法では、合金溶湯を、高
速回転する銅や鉄のロールに噴射することにより、10
5°C/sec以上という非常に早い冷却速度を得、非
晶質もしくは非晶質と結晶質が混在した状態の合金を得
る。この場合、適度な冷却速度を選択することによって
高い保磁力を得ることができる。またさらに高速で急冷
して適度の熱処理をすることにより高保磁力を得ること
ができる。得られた合金の形状はリボン状であり、磁気
的には等方性である。この等方性リボン状合金を永久磁
石として用いる為には、リボンを粉砕し、樹脂と混合し
、成型し樹脂磁石とするか、あるいはホットプレスによ
って高密度化をはかりブロック磁石とする。GM社が特
開昭60−100402号公報に発表したところによる
と、そのブロックを、ダイアンプセントという工法によ
り、異方性ができるとされている。Various manufacturing methods have been proposed for R-Fe-B magnets, but they can be broadly classified into the following two types. One method uses a high-speed quenching method published in Japanese Patent Application Laid-Open No. 59-64739. In this method, molten alloy is injected onto a copper or iron roll rotating at high speed.
A very fast cooling rate of 5°C/sec or more is obtained, and an alloy in an amorphous state or a mixed state of amorphous and crystalline materials is obtained. In this case, a high coercive force can be obtained by selecting an appropriate cooling rate. Furthermore, high coercive force can be obtained by rapidly cooling at a higher speed and performing appropriate heat treatment. The shape of the obtained alloy is ribbon-like and magnetically isotropic. In order to use this isotropic ribbon-shaped alloy as a permanent magnet, the ribbon is crushed, mixed with resin, and molded to form a resin magnet, or it is densified by hot pressing to form a scale block magnet. According to GM's publication in Japanese Patent Laid-Open No. 60-100402, it is said that the block can be made anisotropic by a construction method called die ampscent.
第2の方法は、特開昭59−46008号公報に発表さ
れた粉末冶金焼結法であり、この方法では、従来から一
般的に用いられている粉末冶金法を利用して、溶解鋳造
によって得られた合金鋳塊を粉砕し、成型し、焼結し、
時効する工程を行なって永久磁石を得る。磁界を印加し
ながら成型を行なうので異方性化した磁石が得られる。The second method is the powder metallurgy sintering method announced in Japanese Patent Application Laid-Open No. 59-46008. The obtained alloy ingot is crushed, molded, sintered,
A permanent magnet is obtained by performing an aging process. Since molding is performed while applying a magnetic field, an anisotropic magnet can be obtained.
この方法で保磁力が合金に付与される工程は焼結工程で
あり、鋳塊製造工程での磁気特性は磁石としての特性を
示しておらない。The process in which coercive force is imparted to the alloy in this method is a sintering process, and the magnetic properties in the ingot manufacturing process do not exhibit properties as a magnet.
上述のように、R−Fe−B系磁石は、従来高速急冷法
あるいは粉末冶金焼結法の何れかにより製造されていた
。周知のアルニコ磁石は鋳造法により製造されているが
、R−Fe−B系磁石を鋳造法で製造し、高性能を付与
する方法は従来知られていなかった。このため、鋳造法
によれば容易に対応できる需要家からの要請に充分に対
応できず、また高速急冷設備、プレス等の設備が必要と
なり、工程が長いなどの問題があった。As mentioned above, R-Fe-B magnets have conventionally been manufactured by either a high-speed quenching method or a powder metallurgy sintering method. Although well-known alnico magnets are manufactured by a casting method, there has been no known method for manufacturing R-Fe-B magnets by a casting method and imparting high performance. For this reason, it is not possible to sufficiently meet the demands of customers, which can be easily met by the casting method, and there are also problems such as requiring equipment such as high-speed quenching equipment and a press, resulting in a long process.
アルニコ磁石は、周知のように、Fe−Al−Ni−C
oおよび添加物からなり、合金溶湯を鋳造することによ
り磁石特性を付与されている。場合によっては、高特性
化の為、鋳造体をさらに熱処理する場合もあるが、基本
的磁石特性は鋳造後に具備している。本発明者らは、R
−Fe−B系磁石にあってもアルニコ磁石と同様に鋳造
後に基本的磁石特性を具備している磁石を提供すること
を目的として研究を行なった。As is well known, alnico magnets are Fe-Al-Ni-C
It consists of o and additives, and is given magnetic properties by casting a molten alloy. In some cases, the cast body may be further heat treated to improve its properties, but the basic magnetic properties are maintained after casting. The inventors have discovered that R
Research was conducted with the aim of providing -Fe-B magnets that, like alnico magnets, have basic magnetic properties after casting.
なお、アルニコ磁石は、等方性のもので2.5MGOe
、異方性のものでも10MGOeのエネルギ積しか有さ
す、また保磁力については1.5 KO,以下という低
い値しか有さない。よって、鋳造R−Fe−B系磁石の
磁気特性はアルニコのものを凌ぐものでなければ、磁気
特性上の優位性はない。ところが従来は鋳造法でアルニ
コ磁石に匹敵するR−Fe−B系磁石は得られていなか
った。すなわち、超高速冷却しなければ磁石特性は得ら
れなかった。In addition, the alnico magnet is isotropic and has a value of 2.5 MGOe.
Even the anisotropic one has an energy product of only 10 MGOe, and the coercive force has a low value of less than 1.5 KO. Therefore, unless the magnetic properties of cast R-Fe-B magnets exceed those of alnico, there is no superiority in terms of magnetic properties. However, conventionally, R-Fe-B magnets comparable to alnico magnets have not been obtained by casting methods. In other words, magnetic properties could not be obtained without ultra-high-speed cooling.
C問題点を解決するための手段〕
本発明者らは、R−Fe−B系磁石の組成限定および添
加物の種類と量の限定により鋳造法が適用可能になるこ
とを見出した。Means for Solving Problem C] The present inventors have discovered that the casting method can be applied by limiting the composition of the R-Fe-B magnet and limiting the type and amount of additives.
かかる知見に基づいて、本発明はRヶ(FeaCo+−
m)、、−、−、MyB、(ただし、RはYを含む1種
以上の希土類元素、MはAl、 Ni 、 Ti
、 V 、 Cr。Based on this knowledge, the present invention provides R(FeaCo+-
m), -, -, MyB, (where R is one or more rare earth elements including Y, M is Al, Ni, Ti
, V, Cr.
Mn 、Zr 、Nb 、Mo 、Hf 、
Ta 、w、 Cuからなる群から選択された少な
くとも1種の元素、X、y、2は原子比であり、0.0
3≦x≦0.25;0.005≦y≦0.15 ; 0
.02≦z≦0.15 ; 0.5≦a≦1である)な
る組成式で表わされることを特徴とする高性能希土類鋳
造磁石を提供する。Mn, Zr, Nb, Mo, Hf,
At least one element selected from the group consisting of Ta, w, Cu, X, y, 2 are atomic ratios, 0.0
3≦x≦0.25; 0.005≦y≦0.15; 0
.. The present invention provides a high-performance rare earth cast magnet characterized by being represented by the following compositional formula: 02≦z≦0.15; 0.5≦a≦1.
上記組成は従来発表されているR−Fe−B系磁石の組
成と一部重複するが、上記組成範囲内に特徴である。す
なわち、これらの添加元素を加えた場合、無添加合金に
比べ溶湯からの冷却過程における粒成長が抑制され、ひ
いては高保磁力が得られる事を見出したものである。こ
れらの添加元素の中では、特にNb、Zrにおいて効果
が著しい。このような添加元素を加えた場合、高速急冷
法で用いる105℃/sec以上よりも低い速度でさせ
ブロックを作る高速鋳造も保磁力iHcからは好ましい
。鋳造法を使用することにより、複雑な、高速急冷装置
も必要とせず又リボン等の形状制限もなく、所謂粉末冶
金法という何段にも別れた工程を必要としないで、永久
磁石を製造できるようになった。上記組成式中のx、y
、zの第一提供できることである。次に、上記組成式中
のX。Although the above composition partially overlaps with the composition of conventionally published R-Fe-B magnets, it is characterized within the above composition range. That is, it has been found that when these additive elements are added, grain growth during the cooling process from the molten metal is suppressed compared to alloys without additives, and as a result, high coercive force can be obtained. Among these additive elements, Nb and Zr are particularly effective. When such additive elements are added, high-speed casting to produce blocks at a speed lower than the 105° C./sec or higher used in the high-speed quenching method is also preferable from the viewpoint of coercive force iHc. By using the casting method, permanent magnets can be manufactured without the need for complex, high-speed quenching equipment, no restrictions on the shape of ribbons, etc., and without the need for the multiple steps of the so-called powder metallurgy process. It became so. x, y in the above composition formula
, z is the first thing that can be provided. Next, X in the above compositional formula.
y、zの磁気特性面からの限定理由を説明する。The reason for the limitation from the viewpoint of magnetic properties of y and z will be explained.
X(希土類元素の含有量)が0.03より小さいと保磁
力が低下し、一方Xが0.25より大きいと残留磁束密
度(Br)が低下する。y (M元素−Aβ。When X (rare earth element content) is less than 0.03, the coercive force decreases, while when X is greater than 0.25, the residual magnetic flux density (Br) decreases. y (M element-Aβ.
Ni 、Ti 、V、Cr 、Mn 、Zr
、Nb +Mo+Hf 、Ta 、W、Cuか
らなる群から選択された少なくとも1種の元素)が0.
005より小さいと、高い保磁力が得られず、またyが
0.15より大きいと残留磁束密度(Br)が低下する
。2 (ホウ素含有量)が0.02より小さいと保磁力
が低下し、一方2が0.15より大きいと残留磁束密度
(Br)が低下する。このように、x、y、zが所定範
囲外となり、保磁力もしくは残留磁束密度(Br)が低
下すると、R−Fe−B界磁石の磁気特性は、従来の高
速急冷法あるいは粉末冶金焼結法による磁石の磁気特性
より著しく劣るとともに、アルニコ磁石の最大エネルギ
積を下回ることになる。これに対して、x+ V +
2が所定範囲内にあると、鋳造状態のR−Fe−B界磁
石の磁気特性は、従来の高速急冷法あるいは粉末冶金焼
結法で得られたと発表されているそれぞれ14MGOe
および45MGOeの最大エネルギ積の最高値には到達
しないものの、各種用途の永久磁石に要求されている磁
気特性を完全に満足している。Ni, Ti, V, Cr, Mn, Zr
, Nb + Mo + Hf , Ta , W, Cu) is 0.
When y is smaller than 005, high coercive force cannot be obtained, and when y is larger than 0.15, the residual magnetic flux density (Br) decreases. If 2 (boron content) is less than 0.02, the coercive force will decrease, while if 2 is greater than 0.15, the residual magnetic flux density (Br) will decrease. In this way, when x, y, and z are outside the predetermined range and the coercive force or residual magnetic flux density (Br) decreases, the magnetic properties of the R-Fe-B field magnet will change depending on the conventional high-speed quenching method or powder metallurgy sintering method. In addition to being significantly inferior to the magnetic properties of the magnet obtained by the method, it is also lower than the maximum energy product of the alnico magnet. On the other hand, x+ V +
2 is within a predetermined range, the magnetic properties of the R-Fe-B field magnet in the cast state will be 14MGOe, which has been announced to be obtained by the conventional high-speed quenching method or the powder metallurgy sintering method, respectively.
Although it does not reach the highest value of maximum energy product of 45MGOe, it completely satisfies the magnetic properties required of permanent magnets for various uses.
本発明のR−Fe−B界磁石の上記組成において、Fe
をCo(コバルト)で置換し、Fe/傘亭(Fe+Co
)≧0.5とすると、残留磁束密度の温度特性が改良さ
れる。Coの置換量が50原子%を越えると、残留磁束
密度が低下するため好ましくない。In the above composition of the R-Fe-B field magnet of the present invention, Fe
is replaced with Co (cobalt), and Fe/Kasatei (Fe+Co
)≧0.5, the temperature characteristics of residual magnetic flux density are improved. If the amount of Co substitution exceeds 50 atomic %, the residual magnetic flux density will decrease, which is not preferable.
以下、本発明に係るR−Fe−B界磁石の製造法につい
て説明するが、下記説明の方法に限らずいかなる鋳造法
によっても本発明の磁石の製造は可能である。The method for manufacturing the R-Fe-B field magnet according to the present invention will be described below, but the magnet of the present invention can be manufactured by any casting method, not limited to the method described below.
希土類金属、鉄、ホウ素(またはフェロボロン)、遷移
金属からなる原料群から適量を選択し、非酸化性雰囲気
中で溶解し、合金化し、それに連続して鋳型に鋳造し、
鋳塊を得る。鋳型は金型、砂型、シェルモールド、ロス
トワックス、など任意のものであってよい。鋳塊の大き
さは任意であり、また高性能磁石が使用されている自動
車、コンピューター、モーター用部品を鋳塊から製造す
ることができる。An appropriate amount is selected from a raw material group consisting of rare earth metals, iron, boron (or ferroboron), and transition metals, melted in a non-oxidizing atmosphere, alloyed, and then continuously cast into a mold.
Obtain ingot. The mold may be any type such as a metal mold, sand mold, shell mold, lost wax, or the like. The size of the ingot can be arbitrary, and parts for automobiles, computers, and motors in which high-performance magnets are used can be manufactured from the ingot.
鋳塊磁石をさらに高性能化する為に300℃〜900℃
の温度で熱処理を施す工程、その熱処理中に磁場を印加
する工程、製品形状に加工する工程を、適宜附加するこ
とも選択できる。300°C to 900°C to further improve the performance of ingot magnets
It is also possible to choose to add, as appropriate, a step of performing heat treatment at a temperature of , a step of applying a magnetic field during the heat treatment, and a step of processing into a product shape.
得られた磁石はそのままでも、もちろん使用できるが、
−旦適当な粒径に粉砕し、樹脂と混合し成型し、樹脂磁
石とすることも可能である。場合によっては、異方性化
を計る為に、鋳塊を粉砕し、磁界中成型を行ない焼結、
時効を行なうことも可能である。Of course, the obtained magnet can be used as is, but
- It is also possible to make a resin magnet by first pulverizing it to an appropriate particle size, mixing it with a resin, and molding it. In some cases, in order to achieve anisotropy, the ingot is crushed, molded in a magnetic field, and sintered.
It is also possible to carry out a statute of limitations.
のような効果が達成される。 An effect like this is achieved.
(1)低02化の実現−特に粉末冶金焼結5g、による
と粉末を処理する工程が多く、また粉末成形体が高温で
加熱されるため、粉末中の希土類成分の酸化が多く起る
。このため酸化を予め見込んで粉末中の希土類成分の量
を多くしなければならない。(1) Achievement of low 02 - In particular, with powder metallurgy sintering of 5 g, there are many steps to treat the powder, and the powder compact is heated at high temperature, so oxidation of rare earth components in the powder occurs frequently. For this reason, the amount of rare earth components in the powder must be increased in anticipation of oxidation.
ところが本発明によれば、合金化と鋳造という工程のみ
でR−Fe−B界磁石の基本的磁石特性が具備されるた
め、粉末中の希土類成分の酸化が少なくなる(約110
00pp以下)。このため酸化による磁石特性の劣化が
少なくなり、また希土類成分を予め多く配合する必要が
なくなる。また同じ組成で、本性と粉末冶金法を比較す
ると、本性の方が高い残留磁束密度が得られる。However, according to the present invention, the basic magnetic properties of an R-Fe-B field magnet are achieved only through the steps of alloying and casting, so the oxidation of the rare earth components in the powder is reduced (approximately 110
00pp or less). Therefore, deterioration of magnetic properties due to oxidation is reduced, and there is no need to add a large amount of rare earth components in advance. Furthermore, when comparing the original method and the powder metallurgy method with the same composition, the original method yields a higher residual magnetic flux density.
(2)歩留りの向上−粉末冶金焼結法と比較して工程数
が少なくなったことにより歩留が向上する。(2) Improved yield - Compared to the powder metallurgy sintering method, the number of steps is reduced, which improves the yield.
さらに、焼結体は反り、ちしみなどを伴うので、製品形
状にするためには大きな削りしろを必要とするが、本発
明では、鋳型が設計できる形状であれば加工はほんの僅
かしか必要ではない。Furthermore, since sintered bodies tend to warp and crack, large machining allowances are required to make them into product shapes.However, with the present invention, only a small amount of machining is required as long as the mold can be designed into a shape. do not have.
(3)形状の任意性−鋳型の設計は、粉末成型金型や、
ホットプレスの型の設計に比べ任意性があり、製品の形
状の要求に幅広く対応できる。またリボン形状を得る高
速急冷法のように磁石素材(製品)形状が一種に限られ
ることはない。(3) Arbitrariness of shape - The design of the mold is based on the powder molding mold,
It is more flexible than hot press mold designs and can accommodate a wide range of product shape requirements. Furthermore, the shape of the magnet material (product) is not limited to one type, unlike the high-speed quenching method for obtaining a ribbon shape.
以下、実施例によりさらに詳しく本発明を説明する。Hereinafter, the present invention will be explained in more detail with reference to Examples.
表1に組成を示す合金を高周波溶解炉により溶解し、金
型に鋳造した。得られた鋳塊の寸法はφ表1の比較例と
本発明例を対比すると分かるように、組成の限定により
鋳造後の磁石特性が大幅に異なる。An alloy whose composition is shown in Table 1 was melted in a high frequency melting furnace and cast into a mold. The dimensions of the obtained ingots were as follows: As can be seen by comparing the comparative example in Table 1 with the inventive example, the magnetic properties after casting are significantly different due to compositional limitations.
以下余白Margin below
Claims (1)
_−_y_−_zM_yB_z(ただし、RはYを含む
1種以上の希土類元素、MはAl、Ni、Ti、V、C
r、Mn、Zr、Nb、Mo、Hf、Ta、W、Cuか
らなる群から選択された少なくとも1種の元素、x、y
、z、aは原子比であり、0.03≦x≦0.25;0
.005≦y≦0.15;0.02≦z≦0.15;0
.5≦a≦1.0である)なる組成式で表わされること
を特徴とする高性能希土類鋳造磁石。 2、MがZr、Nbの1種であることを特徴とする特許
請求の範囲第1項記載の高性能希土類鋳造磁石。[Claims] 1. R_x(Fe_aCo_1_-_a)_1_-_x
_−_y_−_zM_yB_z (However, R is one or more rare earth elements including Y, M is Al, Ni, Ti, V, C
r, Mn, Zr, Nb, Mo, Hf, Ta, W, at least one element selected from the group consisting of Cu, x, y
, z, a are atomic ratios, 0.03≦x≦0.25;0
.. 005≦y≦0.15;0.02≦z≦0.15;0
.. A high-performance rare earth cast magnet characterized by being represented by the composition formula: 5≦a≦1.0. 2. The high-performance rare earth cast magnet according to claim 1, wherein M is one of Zr and Nb.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61256743A JPS63111602A (en) | 1986-10-30 | 1986-10-30 | High performance rare earth cast magnet |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61256743A JPS63111602A (en) | 1986-10-30 | 1986-10-30 | High performance rare earth cast magnet |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS63111602A true JPS63111602A (en) | 1988-05-16 |
Family
ID=17296824
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61256743A Pending JPS63111602A (en) | 1986-10-30 | 1986-10-30 | High performance rare earth cast magnet |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS63111602A (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02229664A (en) * | 1989-03-02 | 1990-09-12 | Sumitomo Light Metal Ind Ltd | Manufacture of alloy ingot for permanent magnet |
| US4971637A (en) * | 1988-05-26 | 1990-11-20 | Shin-Etsu Chemical Co., Ltd. | Rare earth permanent magnet |
| JPH0498802A (en) * | 1990-08-17 | 1992-03-31 | Fuji Elelctrochem Co Ltd | Permanent magnet |
| US5123979A (en) * | 1989-12-01 | 1992-06-23 | Aimants Ugimag Sa | Alloy for fe nd b type permanent magnet, sintered permanent magnet and process for obtaining it |
-
1986
- 1986-10-30 JP JP61256743A patent/JPS63111602A/en active Pending
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4971637A (en) * | 1988-05-26 | 1990-11-20 | Shin-Etsu Chemical Co., Ltd. | Rare earth permanent magnet |
| JPH02229664A (en) * | 1989-03-02 | 1990-09-12 | Sumitomo Light Metal Ind Ltd | Manufacture of alloy ingot for permanent magnet |
| US5123979A (en) * | 1989-12-01 | 1992-06-23 | Aimants Ugimag Sa | Alloy for fe nd b type permanent magnet, sintered permanent magnet and process for obtaining it |
| JPH0498802A (en) * | 1990-08-17 | 1992-03-31 | Fuji Elelctrochem Co Ltd | Permanent magnet |
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